source: trunk/source/processes/cuts/src/G4RToEConvForElectron.cc@ 1036

Last change on this file since 1036 was 1007, checked in by garnier, 17 years ago

update to geant4.9.2

File size: 6.1 KB
Line 
1//
2// ********************************************************************
3// * License and Disclaimer *
4// * *
5// * The Geant4 software is copyright of the Copyright Holders of *
6// * the Geant4 Collaboration. It is provided under the terms and *
7// * conditions of the Geant4 Software License, included in the file *
8// * LICENSE and available at http://cern.ch/geant4/license . These *
9// * include a list of copyright holders. *
10// * *
11// * Neither the authors of this software system, nor their employing *
12// * institutes,nor the agencies providing financial support for this *
13// * work make any representation or warranty, express or implied, *
14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
21// * any work based on the software) you agree to acknowledge its *
22// * use in resulting scientific publications, and indicate your *
23// * acceptance of all terms of the Geant4 Software license. *
24// ********************************************************************
25//
26//
27// $Id: G4RToEConvForElectron.cc,v 1.5 2006/06/29 19:30:22 gunter Exp $
28// GEANT4 tag $Name: geant4-09-02 $
29//
30//
31// --------------------------------------------------------------
32// GEANT 4 class implementation file/ History:
33// 5 Oct. 2002, H.Kuirashige : Structure created based on object model
34// --------------------------------------------------------------
35
36#include "G4RToEConvForElectron.hh"
37#include "G4ParticleDefinition.hh"
38#include "G4ParticleTable.hh"
39#include "G4Material.hh"
40#include "G4PhysicsLogVector.hh"
41
42#include "G4ios.hh"
43
44G4RToEConvForElectron::G4RToEConvForElectron() : G4VRangeToEnergyConverter()
45{
46 theParticle = G4ParticleTable::GetParticleTable()->FindParticle("e-");
47 if (theParticle ==0) {
48#ifdef G4VERBOSE
49 if (GetVerboseLevel()>0) {
50 G4cout << " G4RToEConvForElectron::G4RToEConvForElectron() ";
51 G4cout << " Electron is not defined !!" << G4endl;
52 }
53#endif
54 }
55}
56
57G4RToEConvForElectron::~G4RToEConvForElectron()
58{
59}
60
61
62// **********************************************************************
63// ************************* ComputeLoss ********************************
64// **********************************************************************
65G4double G4RToEConvForElectron::ComputeLoss(G4double AtomicNumber,
66 G4double KineticEnergy) const
67{
68 static G4double Z;
69 static G4double taul, ionpot, ionpotlog;
70 const G4double cbr1=0.02, cbr2=-5.7e-5, cbr3=1., cbr4=0.072;
71 const G4double Tlow=10.*keV, Thigh=1.*GeV;
72 static G4double bremfactor= 0.1 ;
73
74 G4double Mass = theParticle->GetPDGMass();
75 // calculate dE/dx for electrons
76 if( std::abs(AtomicNumber-Z)>0.1 ) {
77 Z = AtomicNumber;
78 taul = Tlow/Mass;
79 ionpot = 1.6e-5*MeV*std::exp(0.9*std::log(Z))/Mass;
80 ionpotlog = std::log(ionpot);
81 }
82
83
84 G4double tau = KineticEnergy/Mass;
85 G4double dEdx;
86
87 if(tau<taul) {
88 G4double t1 = taul+1.;
89 G4double t2 = taul+2.;
90 G4double tsq = taul*taul;
91 G4double beta2 = taul*t2/(t1*t1);
92 G4double f = 1.-beta2+std::log(tsq/2.)
93 +(0.5+0.25*tsq+(1.+2.*taul)*std::log(0.5))/(t1*t1);
94 dEdx = (std::log(2.*taul+4.)-2.*ionpotlog+f)/beta2;
95 dEdx = twopi_mc2_rcl2*Z*dEdx;
96 G4double clow = dEdx*std::sqrt(taul);
97 dEdx = clow/std::sqrt(KineticEnergy/Mass);
98
99 } else {
100 G4double t1 = tau+1.;
101 G4double t2 = tau+2.;
102 G4double tsq = tau*tau;
103 G4double beta2 = tau*t2/(t1*t1);
104 G4double f = 1.-beta2+std::log(tsq/2.)
105 +(0.5+0.25*tsq+(1.+2.*tau)*std::log(0.5))/(t1*t1);
106 dEdx = (std::log(2.*tau+4.)-2.*ionpotlog+f)/beta2;
107 dEdx = twopi_mc2_rcl2*Z*dEdx;
108
109 // loss from bremsstrahlung follows
110 G4double cbrem = (cbr1+cbr2*Z)
111 *(cbr3+cbr4*std::log(KineticEnergy/Thigh));
112 cbrem = Z*(Z+1.)*cbrem*tau/beta2;
113
114 cbrem *= bremfactor ;
115
116 dEdx += twopi_mc2_rcl2*cbrem;
117 }
118
119 return dEdx;
120}
121
122
123void G4RToEConvForElectron::BuildRangeVector(const G4Material* aMaterial,
124 G4double maxEnergy,
125 G4double aMass,
126 G4PhysicsLogVector* rangeVector)
127{
128 // create range vector for a material
129 const G4double tlim = 10.*keV;
130 const G4int maxnbint = 100;
131
132 const G4ElementVector* elementVector = aMaterial->GetElementVector();
133 const G4double* atomicNumDensityVector = aMaterial->GetAtomicNumDensityVector();
134 G4int NumEl = aMaterial->GetNumberOfElements();
135
136 // calculate parameters of the low energy part first
137 size_t i;
138 G4double loss=0.;
139 for (i=0; i<size_t(NumEl); i++) {
140 G4bool isOut;
141 G4int IndEl = (*elementVector)[i]->GetIndex();
142 loss += atomicNumDensityVector[i]*
143 (*theLossTable)[IndEl]->GetValue(tlim,isOut);
144 }
145 G4double taulim = tlim/aMass;
146 G4double clim = std::sqrt(taulim)*loss;
147 G4double taumax = maxEnergy/aMass;
148
149 // now the range vector can be filled
150 for ( i=0; i<size_t(TotBin); i++) {
151 G4double LowEdgeEnergy = rangeVector->GetLowEdgeEnergy(i);
152 G4double tau = LowEdgeEnergy/aMass;
153
154 if ( tau <= taulim ) {
155 G4double Value = 2.*aMass*tau*std::sqrt(tau)/(3.*clim);
156 rangeVector->PutValue(i,Value);
157 } else {
158 G4double rangelim = 2.*aMass*taulim*std::sqrt(taulim)/(3.*clim);
159 G4double ltaulow = std::log(taulim);
160 G4double ltauhigh = std::log(tau);
161 G4double ltaumax = std::log(taumax);
162 G4int nbin = G4int(maxnbint*(ltauhigh-ltaulow)/(ltaumax-ltaulow));
163 if( nbin < 1 ) nbin = 1;
164 G4double Value = RangeLogSimpson( NumEl, elementVector,
165 atomicNumDensityVector, aMass,
166 ltaulow, ltauhigh, nbin)
167 + rangelim;
168 rangeVector->PutValue(i,Value);
169 }
170 }
171}
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